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Last updated on 2021-02-17 13:46
Search for electroweak production of charginos and sleptons decaying into final states with two leptons and missing transverse momentum in $\sqrt{s}=13$ TeV $pp$ collisions using the ATLAS detector
A search for the electroweak production of charginos and sleptons decaying into final states with two electrons or muons is presented. The analysis is based on 139.0 fb$^{-1}$ of proton-proton collisions recorded by the ATLAS detector at the Large Hadron Collider at $\sqrt{s}$ = 13 TeV. Three R-parity conserving scenarios where the lightest neutralino is the lightest supersymmetric particle are considered: the production of chargino pairs with decays via either W bosons or sleptons, and the direct production of slepton pairs. The analysis is optimised to target the first of these scenarios, but its results are also interpreted in the other ones. No significant deviations from the Standard Model expectations are observed and stringent limits at 95% confidence level are set on the masses of relevant supersymmetric particles in each of these scenarios. For a massless lightest neutralino, masses up to 420 GeV are excluded for the production of the lightest chargino pairs assuming W boson mediated decays and up to 1 TeV for slepton mediated decays, whereas for slepton-pair production masses up to 700 GeV are excluded assuming three generations of mass-degenerate sleptons.
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Background fit 1
Data from Table 5
10.17182/hepdata.89413.v2/t2
Observed events and predicted background yields from the fit for the CRs. For backgrounds whose normalisation is extracted from the...
Background fit 2
Data from Table 6
10.17182/hepdata.89413.v2/t3
Observed events and predicted post-fit background yields in the VRs. For backgrounds whose normalisation is extracted from the fit in...
VR kinematics 1
Data from Figure 3a
10.17182/hepdata.89413.v2/t4
Distributions of $m_{T2}$ in VR-top-low for data and the estimated SM backgrounds. The normalisation factors extracted from the corresponding CRs...
VR kinematics 2
Data from Figure 3b
10.17182/hepdata.89413.v2/t5
Distributions of $m_{T2}$ in VR-top-high for data and the estimated SM backgrounds. The normalisation factors extracted from the corresponding CRs...
VR kinematics 3
Data from Figure 3c
10.17182/hepdata.89413.v2/t6
Distributions of $E_T^{miss}$ in VR-WW-0J for data and the estimated SM backgrounds. The normalisation factors extracted from the corresponding CRs...
VR kinematics 4
Data from Figure 3d
10.17182/hepdata.89413.v2/t7
Distributions of $E_T^{miss}$ in VR-WW-1J for data and the estimated SM backgrounds. The normalisation factors extracted from the corresponding CRs...
VR kinematics 5
Data from Figure 3e
10.17182/hepdata.89413.v2/t8
Distributions of $E_T^{miss}$ significance in VR-VZ for data and the estimated SM backgrounds. The normalisation factors extracted from the corresponding...
VR kinematics 6
Data from Figure 3f
10.17182/hepdata.89413.v2/t9
Distributions of $E_T^{miss}$ significance in VR-top-WW for data and the estimated SM backgrounds. The normalisation factors extracted from the corresponding...
Systematic uncertainties
Data from Table 7
10.17182/hepdata.89413.v2/t10
Breakdown of the dominant systematic uncertainties on background estimates in the inclusive SRs requiring $m_{T2}$>100 GeV after performing the profile...
Background fit 5
Data from Table 8a
10.17182/hepdata.89413.v2/t11
Observed events and predicted post-fit background yields for the DF inclusive SRs. The model independent upper limits at 95% confidence...
Background fit 6
Data from Table 8b
10.17182/hepdata.89413.v2/t12
Observed events and predicted post-fit background yields for the DF inclusive SRs. The model independent upper limits at 95% confidence...
Background fit 3
Data from Table 9a
10.17182/hepdata.89413.v2/t13
Observed events and predicted post-fit background yields for the SF inclusive SRs. The model independent upper limits at 95% confidence...
Background fit 4
Data from Table 9b
10.17182/hepdata.89413.v2/t14
Observed events and predicted post-fit background yields for the SF inclusive SRs. The model independent upper limits at 95% confidence...
SR kinematics 1
Data from Figure 6a
10.17182/hepdata.89413.v2/t15
Distributions of $m_{T2}$ in SRSF-0J for data and the estimated SM backgrounds. The normalisation factors extracted from the corresponding CRs...
SR kinematics 2
Data from Figure 6b
10.17182/hepdata.89413.v2/t16
Distributions of $m_{T2}$ in SRSF-1J for data and the estimated SM backgrounds. The normalisation factors extracted from the corresponding CRs...
SR kinematics 3
Data from Figure 6c
10.17182/hepdata.89413.v2/t17
Distributions of $m_{T2}$ in SRDF-0J for data and the estimated SM backgrounds. The normalisation factors extracted from the corresponding CRs...
SR kinematics 4
Data from Figure 6d
10.17182/hepdata.89413.v2/t18
Distributions of $m_{T2}$ in SRDF-1J for data and the estimated SM backgrounds. The normalisation factors extracted from the corresponding CRs...
Exclusion contour (obs) 1
Data from Figure 7a
10.17182/hepdata.89413.v2/t19
Observed exclusion limits on SUSY simplified models for chargino-pair production with $W$ boson mediated decays. All limits are computed at...
Exclusion contour (exp) 1
Data from Figure 7a
10.17182/hepdata.89413.v2/t20
Expected exclusion limits on SUSY simplified models for chargino-pair production with $W$ boson mediated decays. All limits are computed at...
Exclusion contour (obs) 2
Data from Figure 7b
10.17182/hepdata.89413.v2/t21
Observed exclusion limits on SUSY simplified models for chargino-pair production with slepton/sneutrino mediated mediated decays. The mass relation $m(\tilde{l}_L)=\frac{1}{2}[m(\tilde{\chi}^{\pm}_1 +...
Exclusion contour (exp) 2
Data from Figure 7b
10.17182/hepdata.89413.v2/t22
Expected exclusion limits on SUSY simplified models for chargino-pair production with slepton/sneutrino mediated mediated decays. The mass relation $m(\tilde{l}_L)=\frac{1}{2}[m(\tilde{\chi}^{\pm}_1 +...
Exclusion contour (obs) 3
Data from Figure 7c
10.17182/hepdata.89413.v2/t23
Observed exclusion limits on SUSY simplified models for slepton-pair production. All limits are computed at 95% CL.
Exclusion contour (exp) 3
Data from Figure 7c
10.17182/hepdata.89413.v2/t24
Expected exclusion limits on SUSY simplified models for slepton-pair production. All limits are computed at 95% CL.
Exclusion contour (obs) 6
Data from Figure 8a
10.17182/hepdata.89413.v2/t25
Observed exclusion limits on SUSY simplified models for selectron-pair production, with left and right handed selectron production combined. All limits...
Exclusion contour (exp) 6
Data from Figure 8a
10.17182/hepdata.89413.v2/t26
Expected exclusion limits on SUSY simplified models for selectron-pair production, with left and right handed selectron production combined. All limits...
Exclusion contour (obs) 7
Data from Figure 8a
10.17182/hepdata.89413.v2/t27
Observed exclusion limits on SUSY simplified models for left-handed selectron-pair production. All limits are computed at 95% CL.
Exclusion contour (exp) 7
Data from Figure 8a
10.17182/hepdata.89413.v2/t28
Expected exclusion limits on SUSY simplified models for left-handed selectron-pair production. All limits are computed at 95% CL.
Exclusion contour (obs) 8
Data from Figure 8a
10.17182/hepdata.89413.v2/t29
Observed exclusion limits on SUSY simplified models for right-handed selectron-pair production. All limits are computed at 95% CL.
Exclusion contour (exp) 8
Data from Figure 8a
10.17182/hepdata.89413.v2/t30
Expected exclusion limits on SUSY simplified models for right-handed selectron-pair production. All limits are computed at 95% CL.
Exclusion contour (obs) 9
Data from Figure 8b
10.17182/hepdata.89413.v2/t31
Observed exclusion limits on SUSY simplified models for smuon-pair production, with left and right handed smuon production combined. All limits...
Exclusion contour (exp) 9
Data from Figure 8b
10.17182/hepdata.89413.v2/t32
Expected exclusion limits on SUSY simplified models for smuon-pair production, with left and right handed smuon production combined. All limits...
Exclusion contour (obs) 10
Data from Figure 8b
10.17182/hepdata.89413.v2/t33
Observed exclusion limits on SUSY simplified models for left-handed smuon-pair production. All limits are computed at 95% CL.
Exclusion contour (exp) 10
Data from Figure 8b
10.17182/hepdata.89413.v2/t34
Expected exclusion limits on SUSY simplified models for left-handed smuon-pair production. All limits are computed at 95% CL.
Exclusion contour (obs) 11
Data from Figure 8b
10.17182/hepdata.89413.v2/t35
Observed exclusion limits on SUSY simplified models for right-handed smuon-pair production. All limits are computed at 95% CL.
Exclusion contour (exp) 11
Data from Figure 8b
10.17182/hepdata.89413.v2/t36
Expected exclusion limits on SUSY simplified models for right-handed smuon-pair production. All limits are computed at 95% CL.
Background fit 7
Data from auxiliary Table 1
10.17182/hepdata.89413.v2/t37
Observed events and predicted background yields from the fit in the binned DF SRs with $n_{non-b-tagged jets}=0$. For backgrounds whose...
Background fit 8
Data from auxiliary Table 2
10.17182/hepdata.89413.v2/t38
Observed events and predicted background yields from the fit in the binned DF SRs with $n_{non-b-tagged jets}=1$. For backgrounds whose...
Background fit 9
Data from auxiliary Table 3
10.17182/hepdata.89413.v2/t39
Observed events and predicted background yields from the fit in the binned SF SRs with $n_{non-b-tagged jets}=0$. For backgrounds whose...
Background fit 10
Data from auxiliary Table 4
10.17182/hepdata.89413.v2/t40
Observed events and predicted background yields from the fit in the binned SF SRs with $n_{non-b-tagged jets}=1$. For backgrounds whose...
Exclusion contour (obs) 4
Data from auxiliary Figure 1
10.17182/hepdata.89413.v2/t41
Observed exclusion limits on SUSY simplified models for left-handed slepton-pair production. All limits are computed at 95% CL.
Exclusion contour (exp) 4
Data from auxiliary Figure 1
10.17182/hepdata.89413.v2/t42
Expected exclusion limits on SUSY simplified models for left-handed slepton-pair production. All limits are computed at 95% CL.
Exclusion contour (obs) 5
Data from auxiliary Figure 1
10.17182/hepdata.89413.v2/t43
Observed exclusion limits on SUSY simplified models for right-handed slepton-pair production. All limits are computed at 95% CL.
Exclusion contour (exp) 5
Data from auxiliary Figure 1
10.17182/hepdata.89413.v2/t44
Expected exclusion limits on SUSY simplified models for right-handed slepton-pair production. All limits are computed at 95% CL.
xsec upper limits 1
Data from auxiliary Figure 3a
10.17182/hepdata.89413.v2/t45
Upper limits on signal cross-section (fb) for chargino-pair production with W -boson-mediated decays.
xsec upper limits 2
Data from auxiliary Figure 3b
10.17182/hepdata.89413.v2/t46
Upper limits on signal cross-section (fb) for chargino-pair production with slepton/sneutrino-mediated decays. The mass relation $m(\tilde{l}_L)=\frac{1}{2}[m(\tilde{\chi}^{\pm}_1 + m(\tilde{\chi}^{0}_1)]$ is assumed.
xsec upper limits 3
Data from auxiliary Figure 3c
10.17182/hepdata.89413.v2/t47
Upper limits on signal cross-section (fb) for slepton-pair production.
Acceptance SR-SF-0J-[100,inf) for C1C1WW grid
Data from auxiliary Figure 4a
10.17182/hepdata.89413.v2/t48
Signal Acceptance for direct chargino-pair production with W-boson mediated decays in SR-SF-0J-[100,inf).
Efficiency SR-SF-0J-[100,inf) for C1C1WW grid
Data from auxiliary Figure 4b
10.17182/hepdata.89413.v2/t49
Signal Efficiency for direct chargino-pair production with W-boson mediated decays in SR-SF-0J-[100,inf).
Acceptance SR-SF-1J-[100,inf) for C1C1WW grid
Data from auxiliary Figure 4c
10.17182/hepdata.89413.v2/t50
Signal Acceptance for direct chargino-pair production with W-boson mediated decays in SR-SF-1J-[100,inf).
Efficiency SR-SF-1J-[100,inf) for C1C1WW grid
Data from auxiliary Figure 4d
10.17182/hepdata.89413.v2/t51
Signal Efficiency for direct chargino-pair production with W-boson mediated decays in SR-SF-1J-[100,inf).
Acceptance SR-DF-0J-[100,inf) for C1C1WW grid
Data from auxiliary Figure 4e
10.17182/hepdata.89413.v2/t52
Signal Acceptance for direct chargino-pair production with W-boson mediated decays in SR-DF-0J-[100,inf).
Efficiency SR-DF-0J-[100,inf) for C1C1WW grid
Data from auxiliary Figure 4f
10.17182/hepdata.89413.v2/t53
Signal Efficiency for direct chargino-pair production with W-boson mediated decays in SR-DF-0J-[100,inf).
Acceptance SR-DF-1J-[100,inf) for C1C1WW grid
Data from auxiliary Figure 4g
10.17182/hepdata.89413.v2/t54
Signal Acceptance for direct chargino-pair production with W-boson mediated decays in SR-DF-1J-[100,inf).
Efficiency SR-DF-1J-[100,inf) for C1C1WW grid
Data from auxiliary Figure 4h
10.17182/hepdata.89413.v2/t55
Signal Efficiency for direct chargino-pair production with W-boson mediated decays in SR-DF-1J-[100,inf).
Acceptance SR-SF-0J-[160,inf) for C1C1WW grid
Data from auxiliary Figure 5a
10.17182/hepdata.89413.v2/t56
Signal Acceptance for direct chargino-pair production with W-boson mediated decays in SR-SF-0J-[160,inf).
Efficiency SR-SF-0J-[160,inf) for C1C1WW grid
Data from auxiliary Figure 5b
10.17182/hepdata.89413.v2/t57
Signal Efficiency for direct chargino-pair production with W-boson mediated decays in SR-SF-0J-[160,inf).
Acceptance SR-SF-1J-[160,inf) for C1C1WW grid
Data from auxiliary Figure 5c
10.17182/hepdata.89413.v2/t58
Signal Acceptance for direct chargino-pair production with W-boson mediated decays in SR-SF-1J-[160,inf).
Efficiency SR-SF-1J-[160,inf) for C1C1WW grid
Data from auxiliary Figure 5d
10.17182/hepdata.89413.v2/t59
Signal Efficiency for direct chargino-pair production with W-boson mediated decays in SR-SF-1J-[160,inf).
Acceptance SR-DF-0J-[160,inf) for C1C1WW grid
Data from auxiliary Figure 5e
10.17182/hepdata.89413.v2/t60
Signal Acceptance for direct chargino-pair production with W-boson mediated decays in SR-DF-0J-[160,inf).
Efficiency SR-DF-0J-[160,inf) for C1C1WW grid
Data from auxiliary Figure 5f
10.17182/hepdata.89413.v2/t61
Signal Efficiency for direct chargino-pair production with W-boson mediated decays in SR-DF-0J-[160,inf).
Acceptance SR-DF-1J-[160,inf) for C1C1WW grid
Data from auxiliary Figure 5g
10.17182/hepdata.89413.v2/t62
Signal Acceptance for direct chargino-pair production with W-boson mediated decays in SR-DF-1J-[160,inf).
Efficiency SR-DF-1J-[160,inf) for C1C1WW grid
Data from auxiliary Figure 5h
10.17182/hepdata.89413.v2/t63
Signal Efficiency for direct chargino-pair production with W-boson mediated decays in SR-DF-1J-[160,inf).
Acceptance SR-SF-0J-[100,120) for C1C1WW grid
Data from auxiliary Figure 6a
10.17182/hepdata.89413.v2/t64
Signal Acceptance for direct chargino-pair production with W-boson mediated decays in SR-SF-0J-[100,120).
Efficiency SR-SF-0J-[100,120) for C1C1WW grid
Data from auxiliary Figure 6b
10.17182/hepdata.89413.v2/t65
Signal Efficiency for direct chargino-pair production with W-boson mediated decays in SR-SF-0J-[100,120).
Acceptance SR-SF-1J-[100,120) for C1C1WW grid
Data from auxiliary Figure 6c
10.17182/hepdata.89413.v2/t66
Signal Acceptance for direct chargino-pair production with W-boson mediated decays in SR-SF-1J-[100,120).
Efficiency SR-SF-1J-[100,120) for C1C1WW grid
Data from auxiliary Figure 6d
10.17182/hepdata.89413.v2/t67
Signal Efficiency for direct chargino-pair production with W-boson mediated decays in SR-SF-1J-[100,120).
Acceptance SR-DF-0J-[100,120) for C1C1WW grid
Data from auxiliary Figure 6e
10.17182/hepdata.89413.v2/t68
Signal Acceptance for direct chargino-pair production with W-boson mediated decays in SR-DF-0J-[100,120).
Efficiency SR-DF-0J-[100,120) for C1C1WW grid
Data from auxiliary Figure 6f
10.17182/hepdata.89413.v2/t69
Signal Efficiency for direct chargino-pair production with W-boson mediated decays in SR-DF-0J-[100,120).
Acceptance SR-DF-1J-[100,120) for C1C1WW grid
Data from auxiliary Figure 6g
10.17182/hepdata.89413.v2/t70
Signal Acceptance for direct chargino-pair production with W-boson mediated decays in SR-DF-1J-[100,120).
Efficiency SR-DF-1J-[100,120) for C1C1WW grid
Data from auxiliary Figure 6h
10.17182/hepdata.89413.v2/t71
Signal Efficiency for direct chargino-pair production with W-boson mediated decays in SR-DF-1J-[100,120).
Acceptance SR-SF-0J-[120,160) for C1C1WW grid
Data from auxiliary Figure 7a
10.17182/hepdata.89413.v2/t72
Signal Acceptance for direct chargino-pair production with W-boson mediated decays in SR-SF-0J-[120,160).
Efficiency SR-SF-0J-[120,160) for C1C1WW grid
Data from auxiliary Figure 7b
10.17182/hepdata.89413.v2/t73
Signal Efficiency for direct chargino-pair production with W-boson mediated decays in SR-SF-0J-[120,160).
Acceptance SR-SF-1J-[120,160) for C1C1WW grid
Data from auxiliary Figure 7c
10.17182/hepdata.89413.v2/t74
Signal Acceptance for direct chargino-pair production with W-boson mediated decays in SR-SF-1J-[120,160).
Efficiency SR-SF-1J-[120,160) for C1C1WW grid
Data from auxiliary Figure 7d
10.17182/hepdata.89413.v2/t75
Signal Efficiency for direct chargino-pair production with W-boson mediated decays in SR-SF-1J-[120,160).
Acceptance SR-DF-0J-[120,160) for C1C1WW grid
Data from auxiliary Figure 7e
10.17182/hepdata.89413.v2/t76
Signal Acceptance for direct chargino-pair production with W-boson mediated decays in SR-DF-0J-[120,160).
Efficiency SR-DF-0J-[120,160) for C1C1WW grid
Data from auxiliary Figure 7f
10.17182/hepdata.89413.v2/t77
Signal Efficiency for direct chargino-pair production with W-boson mediated decays in SR-DF-0J-[120,160).
Acceptance SR-DF-1J-[120,160) for C1C1WW grid
Data from auxiliary Figure 7g
10.17182/hepdata.89413.v2/t78
Signal Acceptance for direct chargino-pair production with W-boson mediated decays in SR-DF-1J-[120,160).
Efficiency SR-DF-1J-[120,160) for C1C1WW grid
Data from auxiliary Figure 7h
10.17182/hepdata.89413.v2/t79
Signal Efficiency for direct chargino-pair production with W-boson mediated decays in SR-DF-1J-[120,160).
Acceptance SR-SF-0J-[100,105) for C1C1WW grid
Data from auxiliary Figure 8a
10.17182/hepdata.89413.v2/t80
Signal Acceptance for direct chargino-pair production with W-boson mediated decays in SR-SF-0J-[100,105).
Efficiency SR-SF-0J-[100,105) for C1C1WW grid
Data from auxiliary Figure 8b
10.17182/hepdata.89413.v2/t81
Signal Efficiency for direct chargino-pair production with W-boson mediated decays in SR-SF-0J-[100,105).
Acceptance SR-SF-1J-[100,105) for C1C1WW grid
Data from auxiliary Figure 8c
10.17182/hepdata.89413.v2/t82
Signal Acceptance for direct chargino-pair production with W-boson mediated decays in SR-SF-1J-[100,105).
Efficiency SR-SF-1J-[100,105) for C1C1WW grid
Data from auxiliary Figure 8d
10.17182/hepdata.89413.v2/t83
Signal Efficiency for direct chargino-pair production with W-boson mediated decays in SR-SF-1J-[100,105).
Acceptance SR-DF-0J-[100,105) for C1C1WW grid
Data from auxiliary Figure 8e
10.17182/hepdata.89413.v2/t84
Signal Acceptance for direct chargino-pair production with W-boson mediated decays in SR-DF-0J-[100,105).
Efficiency SR-DF-0J-[100,105) for C1C1WW grid
Data from auxiliary Figure 8f
10.17182/hepdata.89413.v2/t85
Signal Efficiency for direct chargino-pair production with W-boson mediated decays in SR-DF-0J-[100,105).
Acceptance SR-DF-1J-[100,105) for C1C1WW grid
Data from auxiliary Figure 8g
10.17182/hepdata.89413.v2/t86
Signal Acceptance for direct chargino-pair production with W-boson mediated decays in SR-DF-1J-[100,105).
Efficiency SR-DF-1J-[100,105) for C1C1WW grid
Data from auxiliary Figure 8h
10.17182/hepdata.89413.v2/t87
Signal Efficiency for direct chargino-pair production with W-boson mediated decays in SR-DF-1J-[100,105).
Acceptance SR-SF-0J-[105,110) for C1C1WW grid
Data from auxiliary Figure 9a
10.17182/hepdata.89413.v2/t88
Signal Acceptance for direct chargino-pair production with W-boson mediated decays in SR-SF-0J-[105,110).
Efficiency SR-SF-0J-[105,110) for C1C1WW grid
Data from auxiliary Figure 9b
10.17182/hepdata.89413.v2/t89
Signal Efficiency for direct chargino-pair production with W-boson mediated decays in SR-SF-0J-[105,110).
Acceptance SR-SF-1J-[105,110) for C1C1WW grid
Data from auxiliary Figure 9c
10.17182/hepdata.89413.v2/t90
Signal Acceptance for direct chargino-pair production with W-boson mediated decays in SR-SF-1J-[105,110).
Efficiency SR-SF-1J-[105,110) for C1C1WW grid
Data from auxiliary Figure 9d
10.17182/hepdata.89413.v2/t91
Signal Efficiency for direct chargino-pair production with W-boson mediated decays in SR-SF-1J-[105,110).
Acceptance SR-DF-0J-[105,110) for C1C1WW grid
Data from auxiliary Figure 9e
10.17182/hepdata.89413.v2/t92
Signal Acceptance for direct chargino-pair production with W-boson mediated decays in SR-DF-0J-[105,110).
Efficiency SR-DF-0J-[105,110) for C1C1WW grid
Data from auxiliary Figure 9f
10.17182/hepdata.89413.v2/t93
Signal Efficiency for direct chargino-pair production with W-boson mediated decays in SR-DF-0J-[105,110).
Acceptance SR-DF-1J-[105,110) for C1C1WW grid
Data from auxiliary Figure 9g
10.17182/hepdata.89413.v2/t94
Signal Acceptance for direct chargino-pair production with W-boson mediated decays in SR-DF-1J-[105,110).
Efficiency SR-DF-1J-[105,110) for C1C1WW grid
Data from auxiliary Figure 9h
10.17182/hepdata.89413.v2/t95
Signal Efficiency for direct chargino-pair production with W-boson mediated decays in SR-DF-1J-[105,110).
Acceptance SR-SF-0J-[110,120) for C1C1WW grid
Data from auxiliary Figure 10a
10.17182/hepdata.89413.v2/t96
Signal Acceptance for direct chargino-pair production with W-boson mediated decays in SR-SF-0J-[110,120).
Efficiency SR-SF-0J-[110,120) for C1C1WW grid
Data from auxiliary Figure 10b
10.17182/hepdata.89413.v2/t97
Signal Efficiency for direct chargino-pair production with W-boson mediated decays in SR-SF-0J-[110,120).
Acceptance SR-SF-1J-[110,120) for C1C1WW grid
Data from auxiliary Figure 10c
10.17182/hepdata.89413.v2/t98
Signal Acceptance for direct chargino-pair production with W-boson mediated decays in SR-SF-1J-[110,120).
Efficiency SR-SF-1J-[110,120) for C1C1WW grid
Data from auxiliary Figure 10d
10.17182/hepdata.89413.v2/t99
Signal Efficiency for direct chargino-pair production with W-boson mediated decays in SR-SF-1J-[110,120).
Acceptance SR-DF-0J-[110,120) for C1C1WW grid
Data from auxiliary Figure 10e
10.17182/hepdata.89413.v2/t100
Signal Acceptance for direct chargino-pair production with W-boson mediated decays in SR-DF-0J-[110,120).
Efficiency SR-DF-0J-[110,120) for C1C1WW grid
Data from auxiliary Figure 10f
10.17182/hepdata.89413.v2/t101
Signal Efficiency for direct chargino-pair production with W-boson mediated decays in SR-DF-0J-[110,120).
Acceptance SR-DF-1J-[110,120) for C1C1WW grid
Data from auxiliary Figure 10g
10.17182/hepdata.89413.v2/t102
Signal Acceptance for direct chargino-pair production with W-boson mediated decays in SR-DF-1J-[110,120).
Efficiency SR-DF-1J-[110,120) for C1C1WW grid
Data from auxiliary Figure 10h
10.17182/hepdata.89413.v2/t103
Signal Efficiency for direct chargino-pair production with W-boson mediated decays in SR-DF-1J-[110,120).
Acceptance SR-SF-0J-[120,140) for C1C1WW grid
Data from auxiliary Figure 11a
10.17182/hepdata.89413.v2/t104
Signal Acceptance for direct chargino-pair production with W-boson mediated decays in SR-SF-0J-[120,140).
Efficiency SR-SF-0J-[120,140) for C1C1WW grid
Data from auxiliary Figure 11b
10.17182/hepdata.89413.v2/t105
Signal Efficiency for direct chargino-pair production with W-boson mediated decays in SR-SF-0J-[120,140).
Acceptance SR-SF-1J-[120,140) for C1C1WW grid
Data from auxiliary Figure 11c
10.17182/hepdata.89413.v2/t106
Signal Acceptance for direct chargino-pair production with W-boson mediated decays in SR-SF-1J-[120,140).
Efficiency SR-SF-1J-[120,140) for C1C1WW grid
Data from auxiliary Figure 11d
10.17182/hepdata.89413.v2/t107
Signal Efficiency for direct chargino-pair production with W-boson mediated decays in SR-SF-1J-[120,140).
Acceptance SR-DF-0J-[120,140) for C1C1WW grid
Data from auxiliary Figure 11e
10.17182/hepdata.89413.v2/t108
Signal Acceptance for direct chargino-pair production with W-boson mediated decays in SR-DF-0J-[120,140).
Efficiency SR-DF-0J-[120,140) for C1C1WW grid
Data from auxiliary Figure 11f
10.17182/hepdata.89413.v2/t109
Signal Efficiency for direct chargino-pair production with W-boson mediated decays in SR-DF-0J-[120,140).
Acceptance SR-DF-1J-[120,140) for C1C1WW grid
Data from auxiliary Figure 11g
10.17182/hepdata.89413.v2/t110
Signal Acceptance for direct chargino-pair production with W-boson mediated decays in SR-DF-1J-[120,140).
Efficiency SR-DF-1J-[120,140) for C1C1WW grid
Data from auxiliary Figure 11h
10.17182/hepdata.89413.v2/t111
Signal Efficiency for direct chargino-pair production with W-boson mediated decays in SR-DF-1J-[120,140).
Acceptance SR-SF-0J-[140,160) for C1C1WW grid
Data from auxiliary Figure 12a
10.17182/hepdata.89413.v2/t112
Signal Acceptance for direct chargino-pair production with W-boson mediated decays in SR-SF-0J-[140,160).
Efficiency SR-SF-0J-[140,160) for C1C1WW grid
Data from auxiliary Figure 12b
10.17182/hepdata.89413.v2/t113
Signal Efficiency for direct chargino-pair production with W-boson mediated decays in SR-SF-0J-[140,160).
Acceptance SR-SF-1J-[140,160) for C1C1WW grid
Data from auxiliary Figure 12c
10.17182/hepdata.89413.v2/t114
Signal Acceptance for direct chargino-pair production with W-boson mediated decays in SR-SF-1J-[140,160).
Efficiency SR-SF-1J-[140,160) for C1C1WW grid
Data from auxiliary Figure 12d
10.17182/hepdata.89413.v2/t115
Signal Efficiency for direct chargino-pair production with W-boson mediated decays in SR-SF-1J-[140,160).
Acceptance SR-DF-0J-[140,160) for C1C1WW grid
Data from auxiliary Figure 12e
10.17182/hepdata.89413.v2/t116
Signal Acceptance for direct chargino-pair production with W-boson mediated decays in SR-DF-0J-[140,160).
Efficiency SR-DF-0J-[140,160) for C1C1WW grid
Data from auxiliary Figure 12f
10.17182/hepdata.89413.v2/t117
Signal Efficiency for direct chargino-pair production with W-boson mediated decays in SR-DF-0J-[140,160).
Acceptance SR-DF-1J-[140,160) for C1C1WW grid
Data from auxiliary Figure 12g
10.17182/hepdata.89413.v2/t118
Signal Acceptance for direct chargino-pair production with W-boson mediated decays in SR-DF-1J-[140,160).
Efficiency SR-DF-1J-[140,160) for C1C1WW grid
Data from auxiliary Figure 12h
10.17182/hepdata.89413.v2/t119
Signal Efficiency for direct chargino-pair production with W-boson mediated decays in SR-DF-1J-[140,160).
Acceptance SR-SF-0J-[160,180) for C1C1WW grid
Data from auxiliary Figure 13a
10.17182/hepdata.89413.v2/t120
Signal Acceptance for direct chargino-pair production with W-boson mediated decays in SR-SF-0J-[160,180).
Efficiency SR-SF-0J-[160,180) for C1C1WW grid
Data from auxiliary Figure 13b
10.17182/hepdata.89413.v2/t121
Signal Efficiency for direct chargino-pair production with W-boson mediated decays in SR-SF-0J-[160,180).
Acceptance SR-SF-1J-[160,180) for C1C1WW grid
Data from auxiliary Figure 13c
10.17182/hepdata.89413.v2/t122
Signal Acceptance for direct chargino-pair production with W-boson mediated decays in SR-SF-1J-[160,180).
Efficiency SR-SF-1J-[160,180) for C1C1WW grid
Data from auxiliary Figure 13d
10.17182/hepdata.89413.v2/t123
Signal Efficiency for direct chargino-pair production with W-boson mediated decays in SR-SF-1J-[160,180).
Acceptance SR-DF-0J-[160,180) for C1C1WW grid
Data from auxiliary Figure 13e
10.17182/hepdata.89413.v2/t124
Signal Acceptance for direct chargino-pair production with W-boson mediated decays in SR-DF-0J-[160,180).
Efficiency SR-DF-0J-[160,180) for C1C1WW grid
Data from auxiliary Figure 13f
10.17182/hepdata.89413.v2/t125
Signal Efficiency for direct chargino-pair production with W-boson mediated decays in SR-DF-0J-[160,180).
Acceptance SR-DF-1J-[160,180) for C1C1WW grid
Data from auxiliary Figure 13g
10.17182/hepdata.89413.v2/t126
Signal Acceptance for direct chargino-pair production with W-boson mediated decays in SR-DF-1J-[160,180).
Efficiency SR-DF-1J-[160,180) for C1C1WW grid
Data from auxiliary Figure 13h
10.17182/hepdata.89413.v2/t127
Signal Efficiency for direct chargino-pair production with W-boson mediated decays in SR-DF-1J-[160,180).
Acceptance SR-SF-0J-[180,220) for C1C1WW grid
Data from auxiliary Figure 14a
10.17182/hepdata.89413.v2/t128
Signal Acceptance for direct chargino-pair production with W-boson mediated decays in SR-SF-0J-[180,220).
Efficiency SR-SF-0J-[180,220) for C1C1WW grid
Data from auxiliary Figure 14b
10.17182/hepdata.89413.v2/t129
Signal Efficiency for direct chargino-pair production with W-boson mediated decays in SR-SF-0J-[180,220).
Acceptance SR-SF-1J-[180,220) for C1C1WW grid
Data from auxiliary Figure 14c
10.17182/hepdata.89413.v2/t130
Signal Acceptance for direct chargino-pair production with W-boson mediated decays in SR-SF-1J-[180,220).
Efficiency SR-SF-1J-[180,220) for C1C1WW grid
Data from auxiliary Figure 14d
10.17182/hepdata.89413.v2/t131
Signal Efficiency for direct chargino-pair production with W-boson mediated decays in SR-SF-1J-[180,220).
Acceptance SR-DF-0J-[180,220) for C1C1WW grid
Data from auxiliary Figure 14e
10.17182/hepdata.89413.v2/t132
Signal Acceptance for direct chargino-pair production with W-boson mediated decays in SR-DF-0J-[180,220).
Efficiency SR-DF-0J-[180,220) for C1C1WW grid
Data from auxiliary Figure 14f
10.17182/hepdata.89413.v2/t133
Signal Efficiency for direct chargino-pair production with W-boson mediated decays in SR-DF-0J-[180,220).
Acceptance SR-DF-1J-[180,220) for C1C1WW grid
Data from auxiliary Figure 14g
10.17182/hepdata.89413.v2/t134
Signal Acceptance for direct chargino-pair production with W-boson mediated decays in SR-DF-1J-[180,220).
Efficiency SR-DF-1J-[180,220) for C1C1WW grid
Data from auxiliary Figure 14h
10.17182/hepdata.89413.v2/t135
Signal Efficiency for direct chargino-pair production with W-boson mediated decays in SR-DF-1J-[180,220).
Acceptance SR-SF-0J-[220,260) for C1C1WW grid
Data from auxiliary Figure 15a
10.17182/hepdata.89413.v2/t136
Signal Acceptance for direct chargino-pair production with W-boson mediated decays in SR-SF-0J-[220,260).
Efficiency SR-SF-0J-[220,260) for C1C1WW grid
Data from auxiliary Figure 15b
10.17182/hepdata.89413.v2/t137
Signal Efficiency for direct chargino-pair production with W-boson mediated decays in SR-SF-0J-[220,260).
Acceptance SR-SF-1J-[220,260) for C1C1WW grid
Data from auxiliary Figure 15c
10.17182/hepdata.89413.v2/t138
Signal Acceptance for direct chargino-pair production with W-boson mediated decays in SR-SF-1J-[220,260).
Efficiency SR-SF-1J-[220,260) for C1C1WW grid
Data from auxiliary Figure 15d
10.17182/hepdata.89413.v2/t139
Signal Efficiency for direct chargino-pair production with W-boson mediated decays in SR-SF-1J-[220,260).
Acceptance SR-DF-0J-[220,260) for C1C1WW grid
Data from auxiliary Figure 15e
10.17182/hepdata.89413.v2/t140
Signal Acceptance for direct chargino-pair production with W-boson mediated decays in SR-DF-0J-[220,260).
Efficiency SR-DF-0J-[220,260) for C1C1WW grid
Data from auxiliary Figure 15f
10.17182/hepdata.89413.v2/t141
Signal Efficiency for direct chargino-pair production with W-boson mediated decays in SR-DF-0J-[220,260).
Acceptance SR-DF-1J-[220,260) for C1C1WW grid
Data from auxiliary Figure 15g
10.17182/hepdata.89413.v2/t142
Signal Acceptance for direct chargino-pair production with W-boson mediated decays in SR-DF-1J-[220,260).
Efficiency SR-DF-1J-[220,260) for C1C1WW grid
Data from auxiliary Figure 15h
10.17182/hepdata.89413.v2/t143
Signal Efficiency for direct chargino-pair production with W-boson mediated decays in SR-DF-1J-[220,260).
Acceptance SR-SF-0J-[260,inf) for C1C1WW grid
Data from auxiliary Figure 16a
10.17182/hepdata.89413.v2/t144
Signal Acceptance for direct chargino-pair production with W-boson mediated decays in SR-SF-0J-[260,inf).
Efficiency SR-SF-0J-[260,inf) for C1C1WW grid
Data from auxiliary Figure 16b
10.17182/hepdata.89413.v2/t145
Signal Efficiency for direct chargino-pair production with W-boson mediated decays in SR-SF-0J-[260,inf).
Acceptance SR-SF-1J-[260,inf) for C1C1WW grid
Data from auxiliary Figure 16c
10.17182/hepdata.89413.v2/t146
Signal Acceptance for direct chargino-pair production with W-boson mediated decays in SR-SF-1J-[260,inf).
Efficiency SR-SF-1J-[260,inf) for C1C1WW grid
Data from auxiliary Figure 16d
10.17182/hepdata.89413.v2/t147
Signal Efficiency for direct chargino-pair production with W-boson mediated decays in SR-SF-1J-[260,inf).
Acceptance SR-DF-0J-[260,inf) for C1C1WW grid
Data from auxiliary Figure 16e
10.17182/hepdata.89413.v2/t148
Signal Acceptance for direct chargino-pair production with W-boson mediated decays in SR-DF-0J-[260,inf).
Efficiency SR-DF-0J-[260,inf) for C1C1WW grid
Data from auxiliary Figure 16f
10.17182/hepdata.89413.v2/t149
Signal Efficiency for direct chargino-pair production with W-boson mediated decays in SR-DF-0J-[260,inf).
Acceptance SR-DF-1J-[260,inf) for C1C1WW grid
Data from auxiliary Figure 16g
10.17182/hepdata.89413.v2/t150
Signal Acceptance for direct chargino-pair production with W-boson mediated decays in SR-DF-1J-[260,inf).
Efficiency SR-DF-1J-[260,inf) for C1C1WW grid
Data from auxiliary Figure 16h
10.17182/hepdata.89413.v2/t151
Signal Efficiency for direct chargino-pair production with W-boson mediated decays in SR-DF-1J-[260,inf).
Cutflow 1
Data from auxiliary Table 5
10.17182/hepdata.89413.v2/t152
Cutflow for supersymmetric model where $\tilde{\chi}_1^{\pm}\tilde{\chi}_1^{\mp}$ decay via $W^{\pm}W^{\mp}$. The masses of the two charginos are 300 GeV, while the...
Cutflow 2
Data from auxiliary Table 6
10.17182/hepdata.89413.v2/t153
Cutflow for supersymmetric model where $\tilde{\chi}_1^{\pm}\tilde{\chi}_1^{\mp}$ decay via slepton-neutrino/sneutrino-lepton pair. The masses of the two charginos are 600 GeV, while...
Cutflow 3
Data from auxiliary Table 7
10.17182/hepdata.89413.v2/t154
Cutflow for supersymmetric model where $\tilde\ell\tilde\ell$ are produced. Only $\tilde{e}$ and $\tilde{\mu}$ are considered in this model. The masses of...
Version 2
modifications: SimpleAnalysis implementation file updated
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When using this data, please cite the original publication:
ATLAS
Collaboration
(2020).
Search for electroweak production of charginos and sleptons decaying into final states with two leptons and missing transverse momentum in $\sqrt{s}=13$ TeV $pp$ collisions using the ATLAS detector. Eur.Phys.J.C 80 (2020) 123.
Search for electroweak production of charginos and sleptons decaying into final states with two leptons and missing transverse momentum in $\sqrt{s}=13$ TeV $pp$ collisions using the ATLAS detector. HEPData (collection).
https://doi.org/10.17182/hepdata.89413
or, if you prefer, a specific version of the
record:
ATLAS
Collaboration
(2021).
Search for electroweak production of charginos and sleptons decaying into final states with two leptons and missing transverse momentum in $\sqrt{s}=13$ TeV $pp$ collisions using the ATLAS detector (Version 2). HEPData (collection).
https://doi.org/10.17182/hepdata.89413.v2
You can also cite the 154 data
tables
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ATLAS
Collaboration
(2021).
“Table 1” of “Search for electroweak production of charginos and sleptons decaying into final states with two leptons and missing transverse momentum in $\sqrt{s}=13$ TeV $pp$ collisions using the ATLAS detector” (Version 2). HEPData (dataset).
https://doi.org/10.17182/hepdata.89413.v2/t1
ATLAS
Collaboration
(2021).
“Background fit 1” of “Search for electroweak production of charginos and sleptons decaying into final states with two leptons and missing transverse momentum in $\sqrt{s}=13$ TeV $pp$ collisions using the ATLAS detector” (Version 2). HEPData (dataset).
https://doi.org/10.17182/hepdata.89413.v2/t2
ATLAS
Collaboration
(2021).
“Background fit 2” of “Search for electroweak production of charginos and sleptons decaying into final states with two leptons and missing transverse momentum in $\sqrt{s}=13$ TeV $pp$ collisions using the ATLAS detector” (Version 2). HEPData (dataset).
https://doi.org/10.17182/hepdata.89413.v2/t3
ATLAS
Collaboration
(2021).
“VR kinematics 1” of “Search for electroweak production of charginos and sleptons decaying into final states with two leptons and missing transverse momentum in $\sqrt{s}=13$ TeV $pp$ collisions using the ATLAS detector” (Version 2). HEPData (dataset).
https://doi.org/10.17182/hepdata.89413.v2/t4
ATLAS
Collaboration
(2021).
“VR kinematics 2” of “Search for electroweak production of charginos and sleptons decaying into final states with two leptons and missing transverse momentum in $\sqrt{s}=13$ TeV $pp$ collisions using the ATLAS detector” (Version 2). HEPData (dataset).
https://doi.org/10.17182/hepdata.89413.v2/t5
ATLAS
Collaboration
(2021).
“VR kinematics 3” of “Search for electroweak production of charginos and sleptons decaying into final states with two leptons and missing transverse momentum in $\sqrt{s}=13$ TeV $pp$ collisions using the ATLAS detector” (Version 2). HEPData (dataset).
https://doi.org/10.17182/hepdata.89413.v2/t6
ATLAS
Collaboration
(2021).
“VR kinematics 4” of “Search for electroweak production of charginos and sleptons decaying into final states with two leptons and missing transverse momentum in $\sqrt{s}=13$ TeV $pp$ collisions using the ATLAS detector” (Version 2). HEPData (dataset).
https://doi.org/10.17182/hepdata.89413.v2/t7
ATLAS
Collaboration
(2021).
“VR kinematics 5” of “Search for electroweak production of charginos and sleptons decaying into final states with two leptons and missing transverse momentum in $\sqrt{s}=13$ TeV $pp$ collisions using the ATLAS detector” (Version 2). HEPData (dataset).
https://doi.org/10.17182/hepdata.89413.v2/t8
ATLAS
Collaboration
(2021).
“VR kinematics 6” of “Search for electroweak production of charginos and sleptons decaying into final states with two leptons and missing transverse momentum in $\sqrt{s}=13$ TeV $pp$ collisions using the ATLAS detector” (Version 2). HEPData (dataset).
https://doi.org/10.17182/hepdata.89413.v2/t9
ATLAS
Collaboration
(2021).
“Systematic uncertainties” of “Search for electroweak production of charginos and sleptons decaying into final states with two leptons and missing transverse momentum in $\sqrt{s}=13$ TeV $pp$ collisions using the ATLAS detector” (Version 2). HEPData (dataset).
https://doi.org/10.17182/hepdata.89413.v2/t10
ATLAS
Collaboration
(2021).
“Background fit 5” of “Search for electroweak production of charginos and sleptons decaying into final states with two leptons and missing transverse momentum in $\sqrt{s}=13$ TeV $pp$ collisions using the ATLAS detector” (Version 2). HEPData (dataset).
https://doi.org/10.17182/hepdata.89413.v2/t11
ATLAS
Collaboration
(2021).
“Background fit 6” of “Search for electroweak production of charginos and sleptons decaying into final states with two leptons and missing transverse momentum in $\sqrt{s}=13$ TeV $pp$ collisions using the ATLAS detector” (Version 2). HEPData (dataset).
https://doi.org/10.17182/hepdata.89413.v2/t12
ATLAS
Collaboration
(2021).
“Background fit 3” of “Search for electroweak production of charginos and sleptons decaying into final states with two leptons and missing transverse momentum in $\sqrt{s}=13$ TeV $pp$ collisions using the ATLAS detector” (Version 2). HEPData (dataset).
https://doi.org/10.17182/hepdata.89413.v2/t13
ATLAS
Collaboration
(2021).
“Background fit 4” of “Search for electroweak production of charginos and sleptons decaying into final states with two leptons and missing transverse momentum in $\sqrt{s}=13$ TeV $pp$ collisions using the ATLAS detector” (Version 2). HEPData (dataset).
https://doi.org/10.17182/hepdata.89413.v2/t14
ATLAS
Collaboration
(2021).
“SR kinematics 1” of “Search for electroweak production of charginos and sleptons decaying into final states with two leptons and missing transverse momentum in $\sqrt{s}=13$ TeV $pp$ collisions using the ATLAS detector” (Version 2). HEPData (dataset).
https://doi.org/10.17182/hepdata.89413.v2/t15
ATLAS
Collaboration
(2021).
“SR kinematics 2” of “Search for electroweak production of charginos and sleptons decaying into final states with two leptons and missing transverse momentum in $\sqrt{s}=13$ TeV $pp$ collisions using the ATLAS detector” (Version 2). HEPData (dataset).
https://doi.org/10.17182/hepdata.89413.v2/t16
ATLAS
Collaboration
(2021).
“SR kinematics 3” of “Search for electroweak production of charginos and sleptons decaying into final states with two leptons and missing transverse momentum in $\sqrt{s}=13$ TeV $pp$ collisions using the ATLAS detector” (Version 2). HEPData (dataset).
https://doi.org/10.17182/hepdata.89413.v2/t17
ATLAS
Collaboration
(2021).
“SR kinematics 4” of “Search for electroweak production of charginos and sleptons decaying into final states with two leptons and missing transverse momentum in $\sqrt{s}=13$ TeV $pp$ collisions using the ATLAS detector” (Version 2). HEPData (dataset).
https://doi.org/10.17182/hepdata.89413.v2/t18
ATLAS
Collaboration
(2021).
“Exclusion contour (obs) 1” of “Search for electroweak production of charginos and sleptons decaying into final states with two leptons and missing transverse momentum in $\sqrt{s}=13$ TeV $pp$ collisions using the ATLAS detector” (Version 2). HEPData (dataset).
https://doi.org/10.17182/hepdata.89413.v2/t19
ATLAS
Collaboration
(2021).
“Exclusion contour (exp) 1” of “Search for electroweak production of charginos and sleptons decaying into final states with two leptons and missing transverse momentum in $\sqrt{s}=13$ TeV $pp$ collisions using the ATLAS detector” (Version 2). HEPData (dataset).
https://doi.org/10.17182/hepdata.89413.v2/t20
ATLAS
Collaboration
(2021).
“Exclusion contour (obs) 2” of “Search for electroweak production of charginos and sleptons decaying into final states with two leptons and missing transverse momentum in $\sqrt{s}=13$ TeV $pp$ collisions using the ATLAS detector” (Version 2). HEPData (dataset).
https://doi.org/10.17182/hepdata.89413.v2/t21
ATLAS
Collaboration
(2021).
“Exclusion contour (exp) 2” of “Search for electroweak production of charginos and sleptons decaying into final states with two leptons and missing transverse momentum in $\sqrt{s}=13$ TeV $pp$ collisions using the ATLAS detector” (Version 2). HEPData (dataset).
https://doi.org/10.17182/hepdata.89413.v2/t22
ATLAS
Collaboration
(2021).
“Exclusion contour (obs) 3” of “Search for electroweak production of charginos and sleptons decaying into final states with two leptons and missing transverse momentum in $\sqrt{s}=13$ TeV $pp$ collisions using the ATLAS detector” (Version 2). HEPData (dataset).
https://doi.org/10.17182/hepdata.89413.v2/t23
ATLAS
Collaboration
(2021).
“Exclusion contour (exp) 3” of “Search for electroweak production of charginos and sleptons decaying into final states with two leptons and missing transverse momentum in $\sqrt{s}=13$ TeV $pp$ collisions using the ATLAS detector” (Version 2). HEPData (dataset).
https://doi.org/10.17182/hepdata.89413.v2/t24
ATLAS
Collaboration
(2021).
“Exclusion contour (obs) 6” of “Search for electroweak production of charginos and sleptons decaying into final states with two leptons and missing transverse momentum in $\sqrt{s}=13$ TeV $pp$ collisions using the ATLAS detector” (Version 2). HEPData (dataset).
https://doi.org/10.17182/hepdata.89413.v2/t25
ATLAS
Collaboration
(2021).
“Exclusion contour (exp) 6” of “Search for electroweak production of charginos and sleptons decaying into final states with two leptons and missing transverse momentum in $\sqrt{s}=13$ TeV $pp$ collisions using the ATLAS detector” (Version 2). HEPData (dataset).
https://doi.org/10.17182/hepdata.89413.v2/t26
ATLAS
Collaboration
(2021).
“Exclusion contour (obs) 7” of “Search for electroweak production of charginos and sleptons decaying into final states with two leptons and missing transverse momentum in $\sqrt{s}=13$ TeV $pp$ collisions using the ATLAS detector” (Version 2). HEPData (dataset).
https://doi.org/10.17182/hepdata.89413.v2/t27
ATLAS
Collaboration
(2021).
“Exclusion contour (exp) 7” of “Search for electroweak production of charginos and sleptons decaying into final states with two leptons and missing transverse momentum in $\sqrt{s}=13$ TeV $pp$ collisions using the ATLAS detector” (Version 2). HEPData (dataset).
https://doi.org/10.17182/hepdata.89413.v2/t28
ATLAS
Collaboration
(2021).
“Exclusion contour (obs) 8” of “Search for electroweak production of charginos and sleptons decaying into final states with two leptons and missing transverse momentum in $\sqrt{s}=13$ TeV $pp$ collisions using the ATLAS detector” (Version 2). HEPData (dataset).
https://doi.org/10.17182/hepdata.89413.v2/t29
ATLAS
Collaboration
(2021).
“Exclusion contour (exp) 8” of “Search for electroweak production of charginos and sleptons decaying into final states with two leptons and missing transverse momentum in $\sqrt{s}=13$ TeV $pp$ collisions using the ATLAS detector” (Version 2). HEPData (dataset).
https://doi.org/10.17182/hepdata.89413.v2/t30
ATLAS
Collaboration
(2021).
“Exclusion contour (obs) 9” of “Search for electroweak production of charginos and sleptons decaying into final states with two leptons and missing transverse momentum in $\sqrt{s}=13$ TeV $pp$ collisions using the ATLAS detector” (Version 2). HEPData (dataset).
https://doi.org/10.17182/hepdata.89413.v2/t31
ATLAS
Collaboration
(2021).
“Exclusion contour (exp) 9” of “Search for electroweak production of charginos and sleptons decaying into final states with two leptons and missing transverse momentum in $\sqrt{s}=13$ TeV $pp$ collisions using the ATLAS detector” (Version 2). HEPData (dataset).
https://doi.org/10.17182/hepdata.89413.v2/t32
ATLAS
Collaboration
(2021).
“Exclusion contour (obs) 10” of “Search for electroweak production of charginos and sleptons decaying into final states with two leptons and missing transverse momentum in $\sqrt{s}=13$ TeV $pp$ collisions using the ATLAS detector” (Version 2). HEPData (dataset).
https://doi.org/10.17182/hepdata.89413.v2/t33
ATLAS
Collaboration
(2021).
“Exclusion contour (exp) 10” of “Search for electroweak production of charginos and sleptons decaying into final states with two leptons and missing transverse momentum in $\sqrt{s}=13$ TeV $pp$ collisions using the ATLAS detector” (Version 2). HEPData (dataset).
https://doi.org/10.17182/hepdata.89413.v2/t34
ATLAS
Collaboration
(2021).
“Exclusion contour (obs) 11” of “Search for electroweak production of charginos and sleptons decaying into final states with two leptons and missing transverse momentum in $\sqrt{s}=13$ TeV $pp$ collisions using the ATLAS detector” (Version 2). HEPData (dataset).
https://doi.org/10.17182/hepdata.89413.v2/t35
ATLAS
Collaboration
(2021).
“Exclusion contour (exp) 11” of “Search for electroweak production of charginos and sleptons decaying into final states with two leptons and missing transverse momentum in $\sqrt{s}=13$ TeV $pp$ collisions using the ATLAS detector” (Version 2). HEPData (dataset).
https://doi.org/10.17182/hepdata.89413.v2/t36
ATLAS
Collaboration
(2021).
“Background fit 7” of “Search for electroweak production of charginos and sleptons decaying into final states with two leptons and missing transverse momentum in $\sqrt{s}=13$ TeV $pp$ collisions using the ATLAS detector” (Version 2). HEPData (dataset).
https://doi.org/10.17182/hepdata.89413.v2/t37
ATLAS
Collaboration
(2021).
“Background fit 8” of “Search for electroweak production of charginos and sleptons decaying into final states with two leptons and missing transverse momentum in $\sqrt{s}=13$ TeV $pp$ collisions using the ATLAS detector” (Version 2). HEPData (dataset).
https://doi.org/10.17182/hepdata.89413.v2/t38
ATLAS
Collaboration
(2021).
“Background fit 9” of “Search for electroweak production of charginos and sleptons decaying into final states with two leptons and missing transverse momentum in $\sqrt{s}=13$ TeV $pp$ collisions using the ATLAS detector” (Version 2). HEPData (dataset).
https://doi.org/10.17182/hepdata.89413.v2/t39
ATLAS
Collaboration
(2021).
“Background fit 10” of “Search for electroweak production of charginos and sleptons decaying into final states with two leptons and missing transverse momentum in $\sqrt{s}=13$ TeV $pp$ collisions using the ATLAS detector” (Version 2). HEPData (dataset).
https://doi.org/10.17182/hepdata.89413.v2/t40
ATLAS
Collaboration
(2021).
“Exclusion contour (obs) 4” of “Search for electroweak production of charginos and sleptons decaying into final states with two leptons and missing transverse momentum in $\sqrt{s}=13$ TeV $pp$ collisions using the ATLAS detector” (Version 2). HEPData (dataset).
https://doi.org/10.17182/hepdata.89413.v2/t41
ATLAS
Collaboration
(2021).
“Exclusion contour (exp) 4” of “Search for electroweak production of charginos and sleptons decaying into final states with two leptons and missing transverse momentum in $\sqrt{s}=13$ TeV $pp$ collisions using the ATLAS detector” (Version 2). HEPData (dataset).
https://doi.org/10.17182/hepdata.89413.v2/t42
ATLAS
Collaboration
(2021).
“Exclusion contour (obs) 5” of “Search for electroweak production of charginos and sleptons decaying into final states with two leptons and missing transverse momentum in $\sqrt{s}=13$ TeV $pp$ collisions using the ATLAS detector” (Version 2). HEPData (dataset).
https://doi.org/10.17182/hepdata.89413.v2/t43
ATLAS
Collaboration
(2021).
“Exclusion contour (exp) 5” of “Search for electroweak production of charginos and sleptons decaying into final states with two leptons and missing transverse momentum in $\sqrt{s}=13$ TeV $pp$ collisions using the ATLAS detector” (Version 2). HEPData (dataset).
https://doi.org/10.17182/hepdata.89413.v2/t44
ATLAS
Collaboration
(2021).
“xsec upper limits 1” of “Search for electroweak production of charginos and sleptons decaying into final states with two leptons and missing transverse momentum in $\sqrt{s}=13$ TeV $pp$ collisions using the ATLAS detector” (Version 2). HEPData (dataset).
https://doi.org/10.17182/hepdata.89413.v2/t45
ATLAS
Collaboration
(2021).
“xsec upper limits 2” of “Search for electroweak production of charginos and sleptons decaying into final states with two leptons and missing transverse momentum in $\sqrt{s}=13$ TeV $pp$ collisions using the ATLAS detector” (Version 2). HEPData (dataset).
https://doi.org/10.17182/hepdata.89413.v2/t46
ATLAS
Collaboration
(2021).
“xsec upper limits 3” of “Search for electroweak production of charginos and sleptons decaying into final states with two leptons and missing transverse momentum in $\sqrt{s}=13$ TeV $pp$ collisions using the ATLAS detector” (Version 2). HEPData (dataset).
https://doi.org/10.17182/hepdata.89413.v2/t47
ATLAS
Collaboration
(2021).
“Acceptance SR-SF-0J-[100,inf) for C1C1WW grid” of “Search for electroweak production of charginos and sleptons decaying into final states with two leptons and missing transverse momentum in $\sqrt{s}=13$ TeV $pp$ collisions using the ATLAS detector” (Version 2). HEPData (dataset).
https://doi.org/10.17182/hepdata.89413.v2/t48
ATLAS
Collaboration
(2021).
“Efficiency SR-SF-0J-[100,inf) for C1C1WW grid” of “Search for electroweak production of charginos and sleptons decaying into final states with two leptons and missing transverse momentum in $\sqrt{s}=13$ TeV $pp$ collisions using the ATLAS detector” (Version 2). HEPData (dataset).
https://doi.org/10.17182/hepdata.89413.v2/t49
ATLAS
Collaboration
(2021).
“Acceptance SR-SF-1J-[100,inf) for C1C1WW grid” of “Search for electroweak production of charginos and sleptons decaying into final states with two leptons and missing transverse momentum in $\sqrt{s}=13$ TeV $pp$ collisions using the ATLAS detector” (Version 2). HEPData (dataset).
https://doi.org/10.17182/hepdata.89413.v2/t50
ATLAS
Collaboration
(2021).
“Efficiency SR-SF-1J-[100,inf) for C1C1WW grid” of “Search for electroweak production of charginos and sleptons decaying into final states with two leptons and missing transverse momentum in $\sqrt{s}=13$ TeV $pp$ collisions using the ATLAS detector” (Version 2). HEPData (dataset).
https://doi.org/10.17182/hepdata.89413.v2/t51
ATLAS
Collaboration
(2021).
“Acceptance SR-DF-0J-[100,inf) for C1C1WW grid” of “Search for electroweak production of charginos and sleptons decaying into final states with two leptons and missing transverse momentum in $\sqrt{s}=13$ TeV $pp$ collisions using the ATLAS detector” (Version 2). HEPData (dataset).
https://doi.org/10.17182/hepdata.89413.v2/t52
ATLAS
Collaboration
(2021).
“Efficiency SR-DF-0J-[100,inf) for C1C1WW grid” of “Search for electroweak production of charginos and sleptons decaying into final states with two leptons and missing transverse momentum in $\sqrt{s}=13$ TeV $pp$ collisions using the ATLAS detector” (Version 2). HEPData (dataset).
https://doi.org/10.17182/hepdata.89413.v2/t53
ATLAS
Collaboration
(2021).
“Acceptance SR-DF-1J-[100,inf) for C1C1WW grid” of “Search for electroweak production of charginos and sleptons decaying into final states with two leptons and missing transverse momentum in $\sqrt{s}=13$ TeV $pp$ collisions using the ATLAS detector” (Version 2). HEPData (dataset).
https://doi.org/10.17182/hepdata.89413.v2/t54
ATLAS
Collaboration
(2021).
“Efficiency SR-DF-1J-[100,inf) for C1C1WW grid” of “Search for electroweak production of charginos and sleptons decaying into final states with two leptons and missing transverse momentum in $\sqrt{s}=13$ TeV $pp$ collisions using the ATLAS detector” (Version 2). HEPData (dataset).
https://doi.org/10.17182/hepdata.89413.v2/t55
ATLAS
Collaboration
(2021).
“Acceptance SR-SF-0J-[160,inf) for C1C1WW grid” of “Search for electroweak production of charginos and sleptons decaying into final states with two leptons and missing transverse momentum in $\sqrt{s}=13$ TeV $pp$ collisions using the ATLAS detector” (Version 2). HEPData (dataset).
https://doi.org/10.17182/hepdata.89413.v2/t56
ATLAS
Collaboration
(2021).
“Efficiency SR-SF-0J-[160,inf) for C1C1WW grid” of “Search for electroweak production of charginos and sleptons decaying into final states with two leptons and missing transverse momentum in $\sqrt{s}=13$ TeV $pp$ collisions using the ATLAS detector” (Version 2). HEPData (dataset).
https://doi.org/10.17182/hepdata.89413.v2/t57
ATLAS
Collaboration
(2021).
“Acceptance SR-SF-1J-[160,inf) for C1C1WW grid” of “Search for electroweak production of charginos and sleptons decaying into final states with two leptons and missing transverse momentum in $\sqrt{s}=13$ TeV $pp$ collisions using the ATLAS detector” (Version 2). HEPData (dataset).
https://doi.org/10.17182/hepdata.89413.v2/t58
ATLAS
Collaboration
(2021).
“Efficiency SR-SF-1J-[160,inf) for C1C1WW grid” of “Search for electroweak production of charginos and sleptons decaying into final states with two leptons and missing transverse momentum in $\sqrt{s}=13$ TeV $pp$ collisions using the ATLAS detector” (Version 2). HEPData (dataset).
https://doi.org/10.17182/hepdata.89413.v2/t59
ATLAS
Collaboration
(2021).
“Acceptance SR-DF-0J-[160,inf) for C1C1WW grid” of “Search for electroweak production of charginos and sleptons decaying into final states with two leptons and missing transverse momentum in $\sqrt{s}=13$ TeV $pp$ collisions using the ATLAS detector” (Version 2). HEPData (dataset).
https://doi.org/10.17182/hepdata.89413.v2/t60
ATLAS
Collaboration
(2021).
“Efficiency SR-DF-0J-[160,inf) for C1C1WW grid” of “Search for electroweak production of charginos and sleptons decaying into final states with two leptons and missing transverse momentum in $\sqrt{s}=13$ TeV $pp$ collisions using the ATLAS detector” (Version 2). HEPData (dataset).
https://doi.org/10.17182/hepdata.89413.v2/t61
ATLAS
Collaboration
(2021).
“Acceptance SR-DF-1J-[160,inf) for C1C1WW grid” of “Search for electroweak production of charginos and sleptons decaying into final states with two leptons and missing transverse momentum in $\sqrt{s}=13$ TeV $pp$ collisions using the ATLAS detector” (Version 2). HEPData (dataset).
https://doi.org/10.17182/hepdata.89413.v2/t62
ATLAS
Collaboration
(2021).
“Efficiency SR-DF-1J-[160,inf) for C1C1WW grid” of “Search for electroweak production of charginos and sleptons decaying into final states with two leptons and missing transverse momentum in $\sqrt{s}=13$ TeV $pp$ collisions using the ATLAS detector” (Version 2). HEPData (dataset).
https://doi.org/10.17182/hepdata.89413.v2/t63
ATLAS
Collaboration
(2021).
“Acceptance SR-SF-0J-[100,120) for C1C1WW grid” of “Search for electroweak production of charginos and sleptons decaying into final states with two leptons and missing transverse momentum in $\sqrt{s}=13$ TeV $pp$ collisions using the ATLAS detector” (Version 2). HEPData (dataset).
https://doi.org/10.17182/hepdata.89413.v2/t64
ATLAS
Collaboration
(2021).
“Efficiency SR-SF-0J-[100,120) for C1C1WW grid” of “Search for electroweak production of charginos and sleptons decaying into final states with two leptons and missing transverse momentum in $\sqrt{s}=13$ TeV $pp$ collisions using the ATLAS detector” (Version 2). HEPData (dataset).
https://doi.org/10.17182/hepdata.89413.v2/t65
ATLAS
Collaboration
(2021).
“Acceptance SR-SF-1J-[100,120) for C1C1WW grid” of “Search for electroweak production of charginos and sleptons decaying into final states with two leptons and missing transverse momentum in $\sqrt{s}=13$ TeV $pp$ collisions using the ATLAS detector” (Version 2). HEPData (dataset).
https://doi.org/10.17182/hepdata.89413.v2/t66
ATLAS
Collaboration
(2021).
“Efficiency SR-SF-1J-[100,120) for C1C1WW grid” of “Search for electroweak production of charginos and sleptons decaying into final states with two leptons and missing transverse momentum in $\sqrt{s}=13$ TeV $pp$ collisions using the ATLAS detector” (Version 2). HEPData (dataset).
https://doi.org/10.17182/hepdata.89413.v2/t67
ATLAS
Collaboration
(2021).
“Acceptance SR-DF-0J-[100,120) for C1C1WW grid” of “Search for electroweak production of charginos and sleptons decaying into final states with two leptons and missing transverse momentum in $\sqrt{s}=13$ TeV $pp$ collisions using the ATLAS detector” (Version 2). HEPData (dataset).
https://doi.org/10.17182/hepdata.89413.v2/t68
ATLAS
Collaboration
(2021).
“Efficiency SR-DF-0J-[100,120) for C1C1WW grid” of “Search for electroweak production of charginos and sleptons decaying into final states with two leptons and missing transverse momentum in $\sqrt{s}=13$ TeV $pp$ collisions using the ATLAS detector” (Version 2). HEPData (dataset).
https://doi.org/10.17182/hepdata.89413.v2/t69
ATLAS
Collaboration
(2021).
“Acceptance SR-DF-1J-[100,120) for C1C1WW grid” of “Search for electroweak production of charginos and sleptons decaying into final states with two leptons and missing transverse momentum in $\sqrt{s}=13$ TeV $pp$ collisions using the ATLAS detector” (Version 2). HEPData (dataset).
https://doi.org/10.17182/hepdata.89413.v2/t70
ATLAS
Collaboration
(2021).
“Efficiency SR-DF-1J-[100,120) for C1C1WW grid” of “Search for electroweak production of charginos and sleptons decaying into final states with two leptons and missing transverse momentum in $\sqrt{s}=13$ TeV $pp$ collisions using the ATLAS detector” (Version 2). HEPData (dataset).
https://doi.org/10.17182/hepdata.89413.v2/t71
ATLAS
Collaboration
(2021).
“Acceptance SR-SF-0J-[120,160) for C1C1WW grid” of “Search for electroweak production of charginos and sleptons decaying into final states with two leptons and missing transverse momentum in $\sqrt{s}=13$ TeV $pp$ collisions using the ATLAS detector” (Version 2). HEPData (dataset).
https://doi.org/10.17182/hepdata.89413.v2/t72
ATLAS
Collaboration
(2021).
“Efficiency SR-SF-0J-[120,160) for C1C1WW grid” of “Search for electroweak production of charginos and sleptons decaying into final states with two leptons and missing transverse momentum in $\sqrt{s}=13$ TeV $pp$ collisions using the ATLAS detector” (Version 2). HEPData (dataset).
https://doi.org/10.17182/hepdata.89413.v2/t73
ATLAS
Collaboration
(2021).
“Acceptance SR-SF-1J-[120,160) for C1C1WW grid” of “Search for electroweak production of charginos and sleptons decaying into final states with two leptons and missing transverse momentum in $\sqrt{s}=13$ TeV $pp$ collisions using the ATLAS detector” (Version 2). HEPData (dataset).
https://doi.org/10.17182/hepdata.89413.v2/t74
ATLAS
Collaboration
(2021).
“Efficiency SR-SF-1J-[120,160) for C1C1WW grid” of “Search for electroweak production of charginos and sleptons decaying into final states with two leptons and missing transverse momentum in $\sqrt{s}=13$ TeV $pp$ collisions using the ATLAS detector” (Version 2). HEPData (dataset).
https://doi.org/10.17182/hepdata.89413.v2/t75
ATLAS
Collaboration
(2021).
“Acceptance SR-DF-0J-[120,160) for C1C1WW grid” of “Search for electroweak production of charginos and sleptons decaying into final states with two leptons and missing transverse momentum in $\sqrt{s}=13$ TeV $pp$ collisions using the ATLAS detector” (Version 2). HEPData (dataset).
https://doi.org/10.17182/hepdata.89413.v2/t76
ATLAS
Collaboration
(2021).
“Efficiency SR-DF-0J-[120,160) for C1C1WW grid” of “Search for electroweak production of charginos and sleptons decaying into final states with two leptons and missing transverse momentum in $\sqrt{s}=13$ TeV $pp$ collisions using the ATLAS detector” (Version 2). HEPData (dataset).
https://doi.org/10.17182/hepdata.89413.v2/t77
ATLAS
Collaboration
(2021).
“Acceptance SR-DF-1J-[120,160) for C1C1WW grid” of “Search for electroweak production of charginos and sleptons decaying into final states with two leptons and missing transverse momentum in $\sqrt{s}=13$ TeV $pp$ collisions using the ATLAS detector” (Version 2). HEPData (dataset).
https://doi.org/10.17182/hepdata.89413.v2/t78
ATLAS
Collaboration
(2021).
“Efficiency SR-DF-1J-[120,160) for C1C1WW grid” of “Search for electroweak production of charginos and sleptons decaying into final states with two leptons and missing transverse momentum in $\sqrt{s}=13$ TeV $pp$ collisions using the ATLAS detector” (Version 2). HEPData (dataset).
https://doi.org/10.17182/hepdata.89413.v2/t79
ATLAS
Collaboration
(2021).
“Acceptance SR-SF-0J-[100,105) for C1C1WW grid” of “Search for electroweak production of charginos and sleptons decaying into final states with two leptons and missing transverse momentum in $\sqrt{s}=13$ TeV $pp$ collisions using the ATLAS detector” (Version 2). HEPData (dataset).
https://doi.org/10.17182/hepdata.89413.v2/t80
ATLAS
Collaboration
(2021).
“Efficiency SR-SF-0J-[100,105) for C1C1WW grid” of “Search for electroweak production of charginos and sleptons decaying into final states with two leptons and missing transverse momentum in $\sqrt{s}=13$ TeV $pp$ collisions using the ATLAS detector” (Version 2). HEPData (dataset).
https://doi.org/10.17182/hepdata.89413.v2/t81
ATLAS
Collaboration
(2021).
“Acceptance SR-SF-1J-[100,105) for C1C1WW grid” of “Search for electroweak production of charginos and sleptons decaying into final states with two leptons and missing transverse momentum in $\sqrt{s}=13$ TeV $pp$ collisions using the ATLAS detector” (Version 2). HEPData (dataset).
https://doi.org/10.17182/hepdata.89413.v2/t82
ATLAS
Collaboration
(2021).
“Efficiency SR-SF-1J-[100,105) for C1C1WW grid” of “Search for electroweak production of charginos and sleptons decaying into final states with two leptons and missing transverse momentum in $\sqrt{s}=13$ TeV $pp$ collisions using the ATLAS detector” (Version 2). HEPData (dataset).
https://doi.org/10.17182/hepdata.89413.v2/t83
ATLAS
Collaboration
(2021).
“Acceptance SR-DF-0J-[100,105) for C1C1WW grid” of “Search for electroweak production of charginos and sleptons decaying into final states with two leptons and missing transverse momentum in $\sqrt{s}=13$ TeV $pp$ collisions using the ATLAS detector” (Version 2). HEPData (dataset).
https://doi.org/10.17182/hepdata.89413.v2/t84
ATLAS
Collaboration
(2021).
“Efficiency SR-DF-0J-[100,105) for C1C1WW grid” of “Search for electroweak production of charginos and sleptons decaying into final states with two leptons and missing transverse momentum in $\sqrt{s}=13$ TeV $pp$ collisions using the ATLAS detector” (Version 2). HEPData (dataset).
https://doi.org/10.17182/hepdata.89413.v2/t85
ATLAS
Collaboration
(2021).
“Acceptance SR-DF-1J-[100,105) for C1C1WW grid” of “Search for electroweak production of charginos and sleptons decaying into final states with two leptons and missing transverse momentum in $\sqrt{s}=13$ TeV $pp$ collisions using the ATLAS detector” (Version 2). HEPData (dataset).
https://doi.org/10.17182/hepdata.89413.v2/t86
ATLAS
Collaboration
(2021).
“Efficiency SR-DF-1J-[100,105) for C1C1WW grid” of “Search for electroweak production of charginos and sleptons decaying into final states with two leptons and missing transverse momentum in $\sqrt{s}=13$ TeV $pp$ collisions using the ATLAS detector” (Version 2). HEPData (dataset).
https://doi.org/10.17182/hepdata.89413.v2/t87
ATLAS
Collaboration
(2021).
“Acceptance SR-SF-0J-[105,110) for C1C1WW grid” of “Search for electroweak production of charginos and sleptons decaying into final states with two leptons and missing transverse momentum in $\sqrt{s}=13$ TeV $pp$ collisions using the ATLAS detector” (Version 2). HEPData (dataset).
https://doi.org/10.17182/hepdata.89413.v2/t88
ATLAS
Collaboration
(2021).
“Efficiency SR-SF-0J-[105,110) for C1C1WW grid” of “Search for electroweak production of charginos and sleptons decaying into final states with two leptons and missing transverse momentum in $\sqrt{s}=13$ TeV $pp$ collisions using the ATLAS detector” (Version 2). HEPData (dataset).
https://doi.org/10.17182/hepdata.89413.v2/t89
ATLAS
Collaboration
(2021).
“Acceptance SR-SF-1J-[105,110) for C1C1WW grid” of “Search for electroweak production of charginos and sleptons decaying into final states with two leptons and missing transverse momentum in $\sqrt{s}=13$ TeV $pp$ collisions using the ATLAS detector” (Version 2). HEPData (dataset).
https://doi.org/10.17182/hepdata.89413.v2/t90
ATLAS
Collaboration
(2021).
“Efficiency SR-SF-1J-[105,110) for C1C1WW grid” of “Search for electroweak production of charginos and sleptons decaying into final states with two leptons and missing transverse momentum in $\sqrt{s}=13$ TeV $pp$ collisions using the ATLAS detector” (Version 2). HEPData (dataset).
https://doi.org/10.17182/hepdata.89413.v2/t91
ATLAS
Collaboration
(2021).
“Acceptance SR-DF-0J-[105,110) for C1C1WW grid” of “Search for electroweak production of charginos and sleptons decaying into final states with two leptons and missing transverse momentum in $\sqrt{s}=13$ TeV $pp$ collisions using the ATLAS detector” (Version 2). HEPData (dataset).
https://doi.org/10.17182/hepdata.89413.v2/t92
ATLAS
Collaboration
(2021).
“Efficiency SR-DF-0J-[105,110) for C1C1WW grid” of “Search for electroweak production of charginos and sleptons decaying into final states with two leptons and missing transverse momentum in $\sqrt{s}=13$ TeV $pp$ collisions using the ATLAS detector” (Version 2). HEPData (dataset).
https://doi.org/10.17182/hepdata.89413.v2/t93
ATLAS
Collaboration
(2021).
“Acceptance SR-DF-1J-[105,110) for C1C1WW grid” of “Search for electroweak production of charginos and sleptons decaying into final states with two leptons and missing transverse momentum in $\sqrt{s}=13$ TeV $pp$ collisions using the ATLAS detector” (Version 2). HEPData (dataset).
https://doi.org/10.17182/hepdata.89413.v2/t94
ATLAS
Collaboration
(2021).
“Efficiency SR-DF-1J-[105,110) for C1C1WW grid” of “Search for electroweak production of charginos and sleptons decaying into final states with two leptons and missing transverse momentum in $\sqrt{s}=13$ TeV $pp$ collisions using the ATLAS detector” (Version 2). HEPData (dataset).
https://doi.org/10.17182/hepdata.89413.v2/t95
ATLAS
Collaboration
(2021).
“Acceptance SR-SF-0J-[110,120) for C1C1WW grid” of “Search for electroweak production of charginos and sleptons decaying into final states with two leptons and missing transverse momentum in $\sqrt{s}=13$ TeV $pp$ collisions using the ATLAS detector” (Version 2). HEPData (dataset).
https://doi.org/10.17182/hepdata.89413.v2/t96
ATLAS
Collaboration
(2021).
“Efficiency SR-SF-0J-[110,120) for C1C1WW grid” of “Search for electroweak production of charginos and sleptons decaying into final states with two leptons and missing transverse momentum in $\sqrt{s}=13$ TeV $pp$ collisions using the ATLAS detector” (Version 2). HEPData (dataset).
https://doi.org/10.17182/hepdata.89413.v2/t97
ATLAS
Collaboration
(2021).
“Acceptance SR-SF-1J-[110,120) for C1C1WW grid” of “Search for electroweak production of charginos and sleptons decaying into final states with two leptons and missing transverse momentum in $\sqrt{s}=13$ TeV $pp$ collisions using the ATLAS detector” (Version 2). HEPData (dataset).
https://doi.org/10.17182/hepdata.89413.v2/t98
ATLAS
Collaboration
(2021).
“Efficiency SR-SF-1J-[110,120) for C1C1WW grid” of “Search for electroweak production of charginos and sleptons decaying into final states with two leptons and missing transverse momentum in $\sqrt{s}=13$ TeV $pp$ collisions using the ATLAS detector” (Version 2). HEPData (dataset).
https://doi.org/10.17182/hepdata.89413.v2/t99
ATLAS
Collaboration
(2021).
“Acceptance SR-DF-0J-[110,120) for C1C1WW grid” of “Search for electroweak production of charginos and sleptons decaying into final states with two leptons and missing transverse momentum in $\sqrt{s}=13$ TeV $pp$ collisions using the ATLAS detector” (Version 2). HEPData (dataset).
https://doi.org/10.17182/hepdata.89413.v2/t100
ATLAS
Collaboration
(2021).
“Efficiency SR-DF-0J-[110,120) for C1C1WW grid” of “Search for electroweak production of charginos and sleptons decaying into final states with two leptons and missing transverse momentum in $\sqrt{s}=13$ TeV $pp$ collisions using the ATLAS detector” (Version 2). HEPData (dataset).
https://doi.org/10.17182/hepdata.89413.v2/t101
ATLAS
Collaboration
(2021).
“Acceptance SR-DF-1J-[110,120) for C1C1WW grid” of “Search for electroweak production of charginos and sleptons decaying into final states with two leptons and missing transverse momentum in $\sqrt{s}=13$ TeV $pp$ collisions using the ATLAS detector” (Version 2). HEPData (dataset).
https://doi.org/10.17182/hepdata.89413.v2/t102
ATLAS
Collaboration
(2021).
“Efficiency SR-DF-1J-[110,120) for C1C1WW grid” of “Search for electroweak production of charginos and sleptons decaying into final states with two leptons and missing transverse momentum in $\sqrt{s}=13$ TeV $pp$ collisions using the ATLAS detector” (Version 2). HEPData (dataset).
https://doi.org/10.17182/hepdata.89413.v2/t103
ATLAS
Collaboration
(2021).
“Acceptance SR-SF-0J-[120,140) for C1C1WW grid” of “Search for electroweak production of charginos and sleptons decaying into final states with two leptons and missing transverse momentum in $\sqrt{s}=13$ TeV $pp$ collisions using the ATLAS detector” (Version 2). HEPData (dataset).
https://doi.org/10.17182/hepdata.89413.v2/t104
ATLAS
Collaboration
(2021).
“Efficiency SR-SF-0J-[120,140) for C1C1WW grid” of “Search for electroweak production of charginos and sleptons decaying into final states with two leptons and missing transverse momentum in $\sqrt{s}=13$ TeV $pp$ collisions using the ATLAS detector” (Version 2). HEPData (dataset).
https://doi.org/10.17182/hepdata.89413.v2/t105
ATLAS
Collaboration
(2021).
“Acceptance SR-SF-1J-[120,140) for C1C1WW grid” of “Search for electroweak production of charginos and sleptons decaying into final states with two leptons and missing transverse momentum in $\sqrt{s}=13$ TeV $pp$ collisions using the ATLAS detector” (Version 2). HEPData (dataset).
https://doi.org/10.17182/hepdata.89413.v2/t106
ATLAS
Collaboration
(2021).
“Efficiency SR-SF-1J-[120,140) for C1C1WW grid” of “Search for electroweak production of charginos and sleptons decaying into final states with two leptons and missing transverse momentum in $\sqrt{s}=13$ TeV $pp$ collisions using the ATLAS detector” (Version 2). HEPData (dataset).
https://doi.org/10.17182/hepdata.89413.v2/t107
ATLAS
Collaboration
(2021).
“Acceptance SR-DF-0J-[120,140) for C1C1WW grid” of “Search for electroweak production of charginos and sleptons decaying into final states with two leptons and missing transverse momentum in $\sqrt{s}=13$ TeV $pp$ collisions using the ATLAS detector” (Version 2). HEPData (dataset).
https://doi.org/10.17182/hepdata.89413.v2/t108
ATLAS
Collaboration
(2021).
“Efficiency SR-DF-0J-[120,140) for C1C1WW grid” of “Search for electroweak production of charginos and sleptons decaying into final states with two leptons and missing transverse momentum in $\sqrt{s}=13$ TeV $pp$ collisions using the ATLAS detector” (Version 2). HEPData (dataset).
https://doi.org/10.17182/hepdata.89413.v2/t109
ATLAS
Collaboration
(2021).
“Acceptance SR-DF-1J-[120,140) for C1C1WW grid” of “Search for electroweak production of charginos and sleptons decaying into final states with two leptons and missing transverse momentum in $\sqrt{s}=13$ TeV $pp$ collisions using the ATLAS detector” (Version 2). HEPData (dataset).
https://doi.org/10.17182/hepdata.89413.v2/t110
ATLAS
Collaboration
(2021).
“Efficiency SR-DF-1J-[120,140) for C1C1WW grid” of “Search for electroweak production of charginos and sleptons decaying into final states with two leptons and missing transverse momentum in $\sqrt{s}=13$ TeV $pp$ collisions using the ATLAS detector” (Version 2). HEPData (dataset).
https://doi.org/10.17182/hepdata.89413.v2/t111
ATLAS
Collaboration
(2021).
“Acceptance SR-SF-0J-[140,160) for C1C1WW grid” of “Search for electroweak production of charginos and sleptons decaying into final states with two leptons and missing transverse momentum in $\sqrt{s}=13$ TeV $pp$ collisions using the ATLAS detector” (Version 2). HEPData (dataset).
https://doi.org/10.17182/hepdata.89413.v2/t112
ATLAS
Collaboration
(2021).
“Efficiency SR-SF-0J-[140,160) for C1C1WW grid” of “Search for electroweak production of charginos and sleptons decaying into final states with two leptons and missing transverse momentum in $\sqrt{s}=13$ TeV $pp$ collisions using the ATLAS detector” (Version 2). HEPData (dataset).
https://doi.org/10.17182/hepdata.89413.v2/t113
ATLAS
Collaboration
(2021).
“Acceptance SR-SF-1J-[140,160) for C1C1WW grid” of “Search for electroweak production of charginos and sleptons decaying into final states with two leptons and missing transverse momentum in $\sqrt{s}=13$ TeV $pp$ collisions using the ATLAS detector” (Version 2). HEPData (dataset).
https://doi.org/10.17182/hepdata.89413.v2/t114
ATLAS
Collaboration
(2021).
“Efficiency SR-SF-1J-[140,160) for C1C1WW grid” of “Search for electroweak production of charginos and sleptons decaying into final states with two leptons and missing transverse momentum in $\sqrt{s}=13$ TeV $pp$ collisions using the ATLAS detector” (Version 2). HEPData (dataset).
https://doi.org/10.17182/hepdata.89413.v2/t115
ATLAS
Collaboration
(2021).
“Acceptance SR-DF-0J-[140,160) for C1C1WW grid” of “Search for electroweak production of charginos and sleptons decaying into final states with two leptons and missing transverse momentum in $\sqrt{s}=13$ TeV $pp$ collisions using the ATLAS detector” (Version 2). HEPData (dataset).
https://doi.org/10.17182/hepdata.89413.v2/t116
ATLAS
Collaboration
(2021).
“Efficiency SR-DF-0J-[140,160) for C1C1WW grid” of “Search for electroweak production of charginos and sleptons decaying into final states with two leptons and missing transverse momentum in $\sqrt{s}=13$ TeV $pp$ collisions using the ATLAS detector” (Version 2). HEPData (dataset).
https://doi.org/10.17182/hepdata.89413.v2/t117
ATLAS
Collaboration
(2021).
“Acceptance SR-DF-1J-[140,160) for C1C1WW grid” of “Search for electroweak production of charginos and sleptons decaying into final states with two leptons and missing transverse momentum in $\sqrt{s}=13$ TeV $pp$ collisions using the ATLAS detector” (Version 2). HEPData (dataset).
https://doi.org/10.17182/hepdata.89413.v2/t118
ATLAS
Collaboration
(2021).
“Efficiency SR-DF-1J-[140,160) for C1C1WW grid” of “Search for electroweak production of charginos and sleptons decaying into final states with two leptons and missing transverse momentum in $\sqrt{s}=13$ TeV $pp$ collisions using the ATLAS detector” (Version 2). HEPData (dataset).
https://doi.org/10.17182/hepdata.89413.v2/t119
ATLAS
Collaboration
(2021).
“Acceptance SR-SF-0J-[160,180) for C1C1WW grid” of “Search for electroweak production of charginos and sleptons decaying into final states with two leptons and missing transverse momentum in $\sqrt{s}=13$ TeV $pp$ collisions using the ATLAS detector” (Version 2). HEPData (dataset).
https://doi.org/10.17182/hepdata.89413.v2/t120
ATLAS
Collaboration
(2021).
“Efficiency SR-SF-0J-[160,180) for C1C1WW grid” of “Search for electroweak production of charginos and sleptons decaying into final states with two leptons and missing transverse momentum in $\sqrt{s}=13$ TeV $pp$ collisions using the ATLAS detector” (Version 2). HEPData (dataset).
https://doi.org/10.17182/hepdata.89413.v2/t121
ATLAS
Collaboration
(2021).
“Acceptance SR-SF-1J-[160,180) for C1C1WW grid” of “Search for electroweak production of charginos and sleptons decaying into final states with two leptons and missing transverse momentum in $\sqrt{s}=13$ TeV $pp$ collisions using the ATLAS detector” (Version 2). HEPData (dataset).
https://doi.org/10.17182/hepdata.89413.v2/t122
ATLAS
Collaboration
(2021).
“Efficiency SR-SF-1J-[160,180) for C1C1WW grid” of “Search for electroweak production of charginos and sleptons decaying into final states with two leptons and missing transverse momentum in $\sqrt{s}=13$ TeV $pp$ collisions using the ATLAS detector” (Version 2). HEPData (dataset).
https://doi.org/10.17182/hepdata.89413.v2/t123
ATLAS
Collaboration
(2021).
“Acceptance SR-DF-0J-[160,180) for C1C1WW grid” of “Search for electroweak production of charginos and sleptons decaying into final states with two leptons and missing transverse momentum in $\sqrt{s}=13$ TeV $pp$ collisions using the ATLAS detector” (Version 2). HEPData (dataset).
https://doi.org/10.17182/hepdata.89413.v2/t124
ATLAS
Collaboration
(2021).
“Efficiency SR-DF-0J-[160,180) for C1C1WW grid” of “Search for electroweak production of charginos and sleptons decaying into final states with two leptons and missing transverse momentum in $\sqrt{s}=13$ TeV $pp$ collisions using the ATLAS detector” (Version 2). HEPData (dataset).
https://doi.org/10.17182/hepdata.89413.v2/t125
ATLAS
Collaboration
(2021).
“Acceptance SR-DF-1J-[160,180) for C1C1WW grid” of “Search for electroweak production of charginos and sleptons decaying into final states with two leptons and missing transverse momentum in $\sqrt{s}=13$ TeV $pp$ collisions using the ATLAS detector” (Version 2). HEPData (dataset).
https://doi.org/10.17182/hepdata.89413.v2/t126
ATLAS
Collaboration
(2021).
“Efficiency SR-DF-1J-[160,180) for C1C1WW grid” of “Search for electroweak production of charginos and sleptons decaying into final states with two leptons and missing transverse momentum in $\sqrt{s}=13$ TeV $pp$ collisions using the ATLAS detector” (Version 2). HEPData (dataset).
https://doi.org/10.17182/hepdata.89413.v2/t127
ATLAS
Collaboration
(2021).
“Acceptance SR-SF-0J-[180,220) for C1C1WW grid” of “Search for electroweak production of charginos and sleptons decaying into final states with two leptons and missing transverse momentum in $\sqrt{s}=13$ TeV $pp$ collisions using the ATLAS detector” (Version 2). HEPData (dataset).
https://doi.org/10.17182/hepdata.89413.v2/t128
ATLAS
Collaboration
(2021).
“Efficiency SR-SF-0J-[180,220) for C1C1WW grid” of “Search for electroweak production of charginos and sleptons decaying into final states with two leptons and missing transverse momentum in $\sqrt{s}=13$ TeV $pp$ collisions using the ATLAS detector” (Version 2). HEPData (dataset).
https://doi.org/10.17182/hepdata.89413.v2/t129
ATLAS
Collaboration
(2021).
“Acceptance SR-SF-1J-[180,220) for C1C1WW grid” of “Search for electroweak production of charginos and sleptons decaying into final states with two leptons and missing transverse momentum in $\sqrt{s}=13$ TeV $pp$ collisions using the ATLAS detector” (Version 2). HEPData (dataset).
https://doi.org/10.17182/hepdata.89413.v2/t130
ATLAS
Collaboration
(2021).
“Efficiency SR-SF-1J-[180,220) for C1C1WW grid” of “Search for electroweak production of charginos and sleptons decaying into final states with two leptons and missing transverse momentum in $\sqrt{s}=13$ TeV $pp$ collisions using the ATLAS detector” (Version 2). HEPData (dataset).
https://doi.org/10.17182/hepdata.89413.v2/t131
ATLAS
Collaboration
(2021).
“Acceptance SR-DF-0J-[180,220) for C1C1WW grid” of “Search for electroweak production of charginos and sleptons decaying into final states with two leptons and missing transverse momentum in $\sqrt{s}=13$ TeV $pp$ collisions using the ATLAS detector” (Version 2). HEPData (dataset).
https://doi.org/10.17182/hepdata.89413.v2/t132
ATLAS
Collaboration
(2021).
“Efficiency SR-DF-0J-[180,220) for C1C1WW grid” of “Search for electroweak production of charginos and sleptons decaying into final states with two leptons and missing transverse momentum in $\sqrt{s}=13$ TeV $pp$ collisions using the ATLAS detector” (Version 2). HEPData (dataset).
https://doi.org/10.17182/hepdata.89413.v2/t133
ATLAS
Collaboration
(2021).
“Acceptance SR-DF-1J-[180,220) for C1C1WW grid” of “Search for electroweak production of charginos and sleptons decaying into final states with two leptons and missing transverse momentum in $\sqrt{s}=13$ TeV $pp$ collisions using the ATLAS detector” (Version 2). HEPData (dataset).
https://doi.org/10.17182/hepdata.89413.v2/t134
ATLAS
Collaboration
(2021).
“Efficiency SR-DF-1J-[180,220) for C1C1WW grid” of “Search for electroweak production of charginos and sleptons decaying into final states with two leptons and missing transverse momentum in $\sqrt{s}=13$ TeV $pp$ collisions using the ATLAS detector” (Version 2). HEPData (dataset).
https://doi.org/10.17182/hepdata.89413.v2/t135
ATLAS
Collaboration
(2021).
“Acceptance SR-SF-0J-[220,260) for C1C1WW grid” of “Search for electroweak production of charginos and sleptons decaying into final states with two leptons and missing transverse momentum in $\sqrt{s}=13$ TeV $pp$ collisions using the ATLAS detector” (Version 2). HEPData (dataset).
https://doi.org/10.17182/hepdata.89413.v2/t136
ATLAS
Collaboration
(2021).
“Efficiency SR-SF-0J-[220,260) for C1C1WW grid” of “Search for electroweak production of charginos and sleptons decaying into final states with two leptons and missing transverse momentum in $\sqrt{s}=13$ TeV $pp$ collisions using the ATLAS detector” (Version 2). HEPData (dataset).
https://doi.org/10.17182/hepdata.89413.v2/t137
ATLAS
Collaboration
(2021).
“Acceptance SR-SF-1J-[220,260) for C1C1WW grid” of “Search for electroweak production of charginos and sleptons decaying into final states with two leptons and missing transverse momentum in $\sqrt{s}=13$ TeV $pp$ collisions using the ATLAS detector” (Version 2). HEPData (dataset).
https://doi.org/10.17182/hepdata.89413.v2/t138
ATLAS
Collaboration
(2021).
“Efficiency SR-SF-1J-[220,260) for C1C1WW grid” of “Search for electroweak production of charginos and sleptons decaying into final states with two leptons and missing transverse momentum in $\sqrt{s}=13$ TeV $pp$ collisions using the ATLAS detector” (Version 2). HEPData (dataset).
https://doi.org/10.17182/hepdata.89413.v2/t139
ATLAS
Collaboration
(2021).
“Acceptance SR-DF-0J-[220,260) for C1C1WW grid” of “Search for electroweak production of charginos and sleptons decaying into final states with two leptons and missing transverse momentum in $\sqrt{s}=13$ TeV $pp$ collisions using the ATLAS detector” (Version 2). HEPData (dataset).
https://doi.org/10.17182/hepdata.89413.v2/t140
ATLAS
Collaboration
(2021).
“Efficiency SR-DF-0J-[220,260) for C1C1WW grid” of “Search for electroweak production of charginos and sleptons decaying into final states with two leptons and missing transverse momentum in $\sqrt{s}=13$ TeV $pp$ collisions using the ATLAS detector” (Version 2). HEPData (dataset).
https://doi.org/10.17182/hepdata.89413.v2/t141
ATLAS
Collaboration
(2021).
“Acceptance SR-DF-1J-[220,260) for C1C1WW grid” of “Search for electroweak production of charginos and sleptons decaying into final states with two leptons and missing transverse momentum in $\sqrt{s}=13$ TeV $pp$ collisions using the ATLAS detector” (Version 2). HEPData (dataset).
https://doi.org/10.17182/hepdata.89413.v2/t142
ATLAS
Collaboration
(2021).
“Efficiency SR-DF-1J-[220,260) for C1C1WW grid” of “Search for electroweak production of charginos and sleptons decaying into final states with two leptons and missing transverse momentum in $\sqrt{s}=13$ TeV $pp$ collisions using the ATLAS detector” (Version 2). HEPData (dataset).
https://doi.org/10.17182/hepdata.89413.v2/t143
ATLAS
Collaboration
(2021).
“Acceptance SR-SF-0J-[260,inf) for C1C1WW grid” of “Search for electroweak production of charginos and sleptons decaying into final states with two leptons and missing transverse momentum in $\sqrt{s}=13$ TeV $pp$ collisions using the ATLAS detector” (Version 2). HEPData (dataset).
https://doi.org/10.17182/hepdata.89413.v2/t144
ATLAS
Collaboration
(2021).
“Efficiency SR-SF-0J-[260,inf) for C1C1WW grid” of “Search for electroweak production of charginos and sleptons decaying into final states with two leptons and missing transverse momentum in $\sqrt{s}=13$ TeV $pp$ collisions using the ATLAS detector” (Version 2). HEPData (dataset).
https://doi.org/10.17182/hepdata.89413.v2/t145
ATLAS
Collaboration
(2021).
“Acceptance SR-SF-1J-[260,inf) for C1C1WW grid” of “Search for electroweak production of charginos and sleptons decaying into final states with two leptons and missing transverse momentum in $\sqrt{s}=13$ TeV $pp$ collisions using the ATLAS detector” (Version 2). HEPData (dataset).
https://doi.org/10.17182/hepdata.89413.v2/t146
ATLAS
Collaboration
(2021).
“Efficiency SR-SF-1J-[260,inf) for C1C1WW grid” of “Search for electroweak production of charginos and sleptons decaying into final states with two leptons and missing transverse momentum in $\sqrt{s}=13$ TeV $pp$ collisions using the ATLAS detector” (Version 2). HEPData (dataset).
https://doi.org/10.17182/hepdata.89413.v2/t147
ATLAS
Collaboration
(2021).
“Acceptance SR-DF-0J-[260,inf) for C1C1WW grid” of “Search for electroweak production of charginos and sleptons decaying into final states with two leptons and missing transverse momentum in $\sqrt{s}=13$ TeV $pp$ collisions using the ATLAS detector” (Version 2). HEPData (dataset).
https://doi.org/10.17182/hepdata.89413.v2/t148
ATLAS
Collaboration
(2021).
“Efficiency SR-DF-0J-[260,inf) for C1C1WW grid” of “Search for electroweak production of charginos and sleptons decaying into final states with two leptons and missing transverse momentum in $\sqrt{s}=13$ TeV $pp$ collisions using the ATLAS detector” (Version 2). HEPData (dataset).
https://doi.org/10.17182/hepdata.89413.v2/t149
ATLAS
Collaboration
(2021).
“Acceptance SR-DF-1J-[260,inf) for C1C1WW grid” of “Search for electroweak production of charginos and sleptons decaying into final states with two leptons and missing transverse momentum in $\sqrt{s}=13$ TeV $pp$ collisions using the ATLAS detector” (Version 2). HEPData (dataset).
https://doi.org/10.17182/hepdata.89413.v2/t150
ATLAS
Collaboration
(2021).
“Efficiency SR-DF-1J-[260,inf) for C1C1WW grid” of “Search for electroweak production of charginos and sleptons decaying into final states with two leptons and missing transverse momentum in $\sqrt{s}=13$ TeV $pp$ collisions using the ATLAS detector” (Version 2). HEPData (dataset).
https://doi.org/10.17182/hepdata.89413.v2/t151
ATLAS
Collaboration
(2021).
“Cutflow 1” of “Search for electroweak production of charginos and sleptons decaying into final states with two leptons and missing transverse momentum in $\sqrt{s}=13$ TeV $pp$ collisions using the ATLAS detector” (Version 2). HEPData (dataset).
https://doi.org/10.17182/hepdata.89413.v2/t152
ATLAS
Collaboration
(2021).
“Cutflow 2” of “Search for electroweak production of charginos and sleptons decaying into final states with two leptons and missing transverse momentum in $\sqrt{s}=13$ TeV $pp$ collisions using the ATLAS detector” (Version 2). HEPData (dataset).
https://doi.org/10.17182/hepdata.89413.v2/t153
ATLAS
Collaboration
(2021).
“Cutflow 3” of “Search for electroweak production of charginos and sleptons decaying into final states with two leptons and missing transverse momentum in $\sqrt{s}=13$ TeV $pp$ collisions using the ATLAS detector” (Version 2). HEPData (dataset).
https://doi.org/10.17182/hepdata.89413.v2/t154
Additional resources
Choose resource:
ATLAS
Collaboration
(2021).
“C1C1WW_300_50_SLHA.dat” of “Search for electroweak production of charginos and sleptons decaying into final states with two leptons and missing transverse momentum in $\sqrt{s}=13$ TeV $pp$ collisions using the ATLAS detector” (Version 2). HEPData (other).
https://doi.org/10.17182/hepdata.89413.v2/r1
ATLAS
Collaboration
(2021).
“C1C1SlepSnu_600_300_1_SLHA.dat” of “Search for electroweak production of charginos and sleptons decaying into final states with two leptons and missing transverse momentum in $\sqrt{s}=13$ TeV $pp$ collisions using the ATLAS detector” (Version 2). HEPData (other).
https://doi.org/10.17182/hepdata.89413.v2/r2
ATLAS
Collaboration
(2021).
“SlepSlep_400_200_SLHA.dat” of “Search for electroweak production of charginos and sleptons decaying into final states with two leptons and missing transverse momentum in $\sqrt{s}=13$ TeV $pp$ collisions using the ATLAS detector” (Version 2). HEPData (other).
https://doi.org/10.17182/hepdata.89413.v2/r3
ATLAS
Collaboration
(2021).
“ANA-SUSY-2018-32.cxx” of “Search for electroweak production of charginos and sleptons decaying into final states with two leptons and missing transverse momentum in $\sqrt{s}=13$ TeV $pp$ collisions using the ATLAS detector” (Version 2). HEPData (other).
https://doi.org/10.17182/hepdata.89413.v2/r4
When using this data, please cite the original publication:
ATLAS
Collaboration
(2020).
Search for electroweak production of charginos and sleptons decaying into final states with two leptons and missing transverse momentum in $\sqrt{s}=13$ TeV $pp$ collisions using the ATLAS detector. Eur.Phys.J.C 80 (2020) 123.
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